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There are some discrepancies in the literature concerning Eq. (61). The form given here when applied to p = 2 and N = 1.333 agrees with Eq. (5) and Table 1 of [28] but does not agree for p=2 and N= 1.333 with Eqs. (4.30), (4.31), and (4.34) of the earlier [24], which were reproduced as Eqs. (5.106) and (5.108) of [30]. The appropriate quantities to expand in Taylor series about the rainbow angle are Eq. (4.29) of [24] and Eq. (5.62) of [31].
-
There are some discrepancies in the literature concerning Eq. (61). The form given here when applied to p = 2 and N = 1.333 agrees with Eq. (5) and Table 1 of [28] but does not agree for p=2 and N= 1.333 with Eqs. (4.30), (4.31), and (4.34) of the earlier [24], which were reproduced as Eqs. (5.106) and (5.108) of [30]. The appropriate quantities to expand in Taylor series about the rainbow angle are Eq. (4.29) of [24] and Eq. (5.62) of [31].
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31
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Most of the results of this paper and of [9,10] were presented in preliminary form at the Fall Meeting of the Ohio Section of the American Physical Society, Cleveland Ohio, October 14-15, 2005.
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Most of the results of this paper and of [9,10] were presented in preliminary form at the Fall Meeting of the Ohio Section of the American Physical Society, Cleveland Ohio, October 14-15, 2005.
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